paper

Chemical potential of a test hard sphere of variable size in hard-sphere fluid mixtures

arXiv:1804.10832 · doi:10.1063/1.5037856

Abstract

A detailed comparison between the Boublík-Mansoori-Carnahan-Starling-Leland (BMCSL)equation of state of hard-sphere mixtures is made with Molecular Dynamics (MD) simulations of the same compositions. The Labík and Smith simulation technique [S. Labík and W. R. Smith, Mol. Simul. \textbf{12}, 23-31 (1994)] was used to implement the Widom particle insertion method to calculate the excess chemical potential, , of a test particle of variable diameter, , immersed in a hard-sphere fluid mixture with different compositions and values of the packing fraction, . Use is made of the fact that the only polynomial representation of which is consistent with the limits and has to be of the cubic form, i.e., , where is the first moment of the distribution. The first two coefficients, and , are known analytically, while and were obtained by fitting the MD data to this expression. This in turn provides a method to determine the excess free energy per particle, , in terms of , , and the compressibility factor, . Very good agreement between the BMCSL formulas and the MD data is found for , , and for binary mixtures and continuous particle size distributions with the top-hat analytic form. However, the BMCSL theory typically slightly underestimates the simulation values, especially for , differences which the Boublík-Carnahan-Starling-Kolafa formulas and an interpolation between two Percus-Yevick routes capture well in different ranges of the system parameter space.

11(+5) pages, 10 figures; Supplementary Material included; v2: slight change in title plus other minor changes